液相二氧化钛纳米微粒的荧光和共振散射光谱特性

以钛酸四丁酯(TBTi)为前驱体,利用微波高压反应法合成了纳米二氧化钛溶胶,并与Ti(SO4)2水解法制备出的二氧化钛纳米微粒对比.考察了两种前驱体制备的二氧化钛纳米微粒荧光光谱及共振散射光谱特性,用TBTi制备的二氧化钛纳米微粒在320 nm有一个共振散射峰,在470 nm有一个同步散射峰,在360,400和470 nm处有三个荧光发射峰;用Ti(SO4)2制备的二氧化钛纳米微粒在340 nm有个共振散射峰,在470 nm有一个同步散射峰,400和470 nm处有两个荧光发射峰.反应条件对共振散射强度的影响与其对荧光的影响变化趋势一致,但共振散射光强度较荧光强度强得多.     

鸟苷发酵不同阶段发酵液紫外特征光谱的研究

研究了发酵不同阶段鸟苷发酵液的紫外吸收光谱,结果表明,鸟苷发酵不同阶段发酵液紫外吸收光谱会呈现相应的特征光谱。发酵前期除了275nm处的波峰外,在249nm又出现了一个新峰,并且随着发酵时间增加新峰逐渐升高成为主峰;发酵中期275nm处的波峰逐渐减弱并最后消失;发酵后期249nm处的波峰成为发酵液的特征波峰,并随时间的增加逐渐上升;发酵末期的显著特征为发酵液λmax的吸光值基本不变。鸟苷发酵不同阶段发酵液特征光谱研究为人们认识鸟苷发酵的动态过程提供了一种新的技术和途径,对于鸟苷发酵生产具有一定的指导意义。     

Broadband light generation at approximately 1300 nm through spectrally recoiled solitons and dispersive waves

We experimentally study the generation of broadband light at approximately 1300 nm from an 810 nm Ti:sapphire femtosecond pump laser. We use two photonic crystal fibers with a second infrared zero-dispersion wavelength (lambda Z2) and compare the efficiency of two schemes: in one fiber lambda Z2=1400 nm and the light at 1300 nm is composed of spectrally recoiled solitons; in the other fiber lambda Z2=1200 nm and the light at 1300 nm is composed of dispersive waves.     

掺镱硅酸盐玻璃的光谱性质

采用高温熔融工艺制备了掺Yb^3＋硅酸盐玻璃。测试了玻璃的吸收光谱和荧光光谱,计算并分析了Yb^3＋离子在975nm附近的吸收截面和积分吸收截面随掺杂浓度的变化趋势。玻璃光谱曲线表明：吸收主峰位于975nm,在900—960nm范围内有一个弥散的吸收峰,中心波长为930nm;荧光主峰位于975nm,荧光次峰位于1010nm。综合其性能表明实验中硅酸盐玻璃的最佳Yb^3＋掺杂浓度为4mol%。     

Dose response of thermoluminescence emission spectra of LiF:Mg,Ti with different Mg, Ti impurity concentrations

The dose response of the TL emission spectra of an LiF:Mg,Ti (TLD-100) sample and three LiF:Mg,Ti samples with different impurity concentrations (0–6 ppm Ti and 80–100 ppm Mg) have been measured. At a dose less than 22 Gy the emission spectrum of the TLD-100 sample comprises one emission band at 420 nm. The sample without Ti shows also one emission band but now at 620 nm. The spectra of the other two samples comprises two emission bands at 420 nm and 620 nm of which the intensity of the 420 nm band increases with increasing Ti concentration. The dose response of the glow peaks is different for peaks at different temperatures and emission bands. From these observations it can be concluded than in LiF:Mg,Ti at least some of the traps and luminescent centers are coupled.     

掺Yb3+激光玻璃光谱特性研究

采用高温熔融工艺制备了Yb3 掺杂激光玻璃.测试了玻璃的吸收光谱和发射光谱,计算了Yb3 的积分吸收截面和受激发射截面及荧光寿命等参数.玻璃光谱曲线表明:吸收主峰位于975.35 nm,在900～962 nm范围内有一较为弥散的吸收次峰,中心波长为939.17nm;荧光主峰位于977.15 nm,荧光次峰位于997.42 m;随着样品厚度的增加,荧光次峰强度和荧光主峰强度在增大,荧光次峰波长和荧光主峰波长向长波方向移动;荧光有效线宽从34.64 nm增大到54.50 nm;荧光寿命由1.04 ms减小为1.00 ms.     

An All-Solid-State Tunable Dual-Wavelength Ti：Sapphire Laser with Quasi-Continuous-Wave Outputs

A high power dual-wavelength Ti：sapphire laser system with wide turning range and high efficiency is described, which consists of two prism-dispersed resonators pumped by an a11-solid-state frequency-doubled Nd：YAG laser. Tunable dual-wavelength outputs, with one wavelength range from 750nm to 795nm and the other from 80Ohm to 850nm, have been demonstrated. With a pump power of 23 W at 532nm, a repetition rate of 6.5kHz and a pulse width of 67.6ns, the maximum dual-wavelength output power of 5.6 W at 785.3nm and 812.1 run, with a pulse width of 17.2ns and a line width of 2nm, has been achieved, leading to an optical-to-optical conversion efficiency of 24.4%.     

氢在碳纳米纤维中的低温吸附储存特性

利用容积法测量了77K下氢在一种碳纳米纤维上的吸附等温线。采用分子模拟的方法模拟了77K下氢分子在平板状碳纳米纤维中的吸附,碳纳米纤维的石墨层层间距分别为0.335nm、0.6nm、0.9nm以及1.5nm。模拟结果表明:石墨层层间距为0.335nm的碳纳米纤维在77K下吸附储氢密度很难达到DOE的能量密度标准;当板间距为0.9nm时,系统吸附储氢的重量密度和体积密度均能达到最大,且在77K、1MPa下,能达到DOE的能量密度标准。     

Electroluminescence in LiNbO3 single crystals

The light emission from LiNbO₃ single crystals caused by the applied a.c. high voltage is studied. It is interpreted as electroluminescence due to impact processes of field accelerated electrons. Two bands can be distinguished in the emission spectrum: one larger with the maximum at 660nm and one smaller at about 500nm.     

动态光散射技术的角度依赖性

与单角度动态光散射技术相比,多角度动态光散射(MDLS)颗粒测量技术能够提高颗粒粒度分布的测量准确性。但在MDLS技术中,测量角度的选择常常与被测颗粒体系的分布有关。对100nm、500nm的单峰模拟分布和300nm与600nm混合的双峰模拟分布的颗粒体系,分别在1、3、6、9个散射角条件下进行了测量。颗粒粒度反演结果表明,随着散射角个数的增大,颗粒粒度分布更趋于真实的颗粒粒度分布。对数量比为5:1的100nm与503nm双峰分布的聚苯乙烯颗粒,分别在1、3、5、10个散射角条件下进行了测量,实测结果表明采用单角度测量只能得到单峰分布,3个及更多散射角可得到双峰分布,并且双峰的数量比随散射角数量的增加逐渐趋近真实的数量比。因此,MDLS颗粒测量技术能够改善颗粒粒度分布的测量结果,但这种改善程度会随散射角的增多逐渐降低。由于散射角个数的增多会增加散射角的校准噪声和光强相关函数的测量噪声,因而会导致在有些情况下颗粒粒度分布的测量结果反而变差。     

高损伤阈值三倍频分离膜

 设计了Nd：YAG激光用三倍频分离膜,膜层材料为SiO₂和HfO₂。经过优化,膜系在355 nm处的反射率在99%以上,在532 nm和1 064 nm处透射率也在99%以上。采用电子束蒸发技术,在熔融石英基底上制备了样品,经测量,制备的分离膜光学性能与设计值接近。分离膜在355 nm激光辐照下的损伤阈值为5.1 J/cm²,并用微分干涉显微镜表征了薄膜损伤形貌。     

Directly diode-pumped Yb:KY(WO(4))(2) regenerative amplifiers

Two Yb(3+) -doped KY(WO(4))(2) regenerative amplifiers, one end pumped by two 1.6-W single-stripe diodes at 940 nm and the other side pumped by one 20-W diode bar at 980 nm, are demonstrated. When the regenerative amplifiers are injected, 40-muJ , 400-fs and 65-muJ , 460-fs pulses at a 1-kHz repetition rate are obtained following compression from the end- and side-pumped amplifiers, respectively.     

Cathodoluminescence in deformed MgO crystals

The corrected cathodoluminescence (CL) emission spectrum for undeformed MgO in the wavelength range 300–650nm consists of two overlapping bands with peaks at 425 nm (2.92 eV) and 488 nm (2.54 eV). After deformation one broad band at 466 nm (2.66 eV) of much higher intensity is observed. In the near IR part of the spectrum a further broad band occurs, consisting of a number of unresolved peaks the strongest of which is at 726 nm (1.71 eV). This band is unaffected by deformation and is thought to be due to iron impurities. Panchromatic and monochromatic SEM micrographs show that the enhanced 466 nm band luminescence comes from the slipped planes of the crystal. Shape analysis of the 466 nm emission band showed that it is a Gaussian form around the intensity maximum with an exponential high energy tail.     

Design of single-material guided-mode resonance filter

In this letter, a guided-mode resonance （GMR） filter with the same material for both the grating layer and the waveguide layer is designed, and its optical properties are investigated. The GMR filter owns almost 100% reflection at the resonance wavelength of 800 nm with the full-width at half-maximum （FWHM） of 20 nm, and its sideband reflection from 700 to 1000 nm is less than 5%. As the resonance wavelength is influenced by more than one parameter during the fabrication process, GMR filter with the same resonance wavelength can be obtained by adjusting other parameters or even one parameter to deviate from the design value.     

LiNbO3:Cr:ZnO晶体生长和光谱特性的研究

采用提拉法从近化学计量比的熔体中生长出尺寸为φ20 mm×50 mm的优质LiNbO3:Cr:ZnO(CZLN)晶体,其光学均匀度为7.59(10-5).进行了吸收和荧光光谱的测定研究.吸收谱测试表明:Cr3 离子在晶体中有2个宽且强的吸收带及1个微弱的吸收线,两宽带中心波长分别为480和660 nm,对应于4A2→4T1和4A2→4T2两个具有相同的总自旋能级之间的跃迁,在4A2→4T2吸收宽带的长波边缘处有个很小的吸收峰,其波长为727nm,对应于4A2→2E(R线)的跃迁.荧光测试表明:当激发波长为660 nm时,CZLN晶体荧光宽带和1个较弱的荧光线峰并存,宽带范围为802～988 nm,峰值波长为871 nm,对应于4T2→2E,4A2的联合能级跃迁,荧光线峰波长约为754 nm,其强度较弱,相应于2E→4A2(零声子线)能级跃迁.计算了晶场强度和Racah参数,其Dq/B=2.72,晶体属于强场介质.研究表明,CZLN晶体具备可调谐激光晶体的基本光谱要求,且有良好的物化性能,可以实现宽频带可调谐激光输出.它又具有较大的倍频系数,有望实现420 nm附近紫外的自倍频激光输出.     

Efficient diode-pumped laser operation of Tm:Lu2O3 around 2 μm

We report on the first diode-pumped laser operation of thulium-doped Lu2O3. With a very compact setup an output power of 75?W and slope efficiencies of around 40% with respect to the incident pump power were achieved at room temperature. Free running laser operation was observed at wavelengths of 2065?nm and 1965?nm. With a birefringent filter the wavelength could continuously be tuned from 1922?nm to 2134?nm. The thermal conductivity of Tm:Lu2O3 was measured for different dopant concentrations and is compared to the one of thulium-doped YAG.     

两种激发波长下蔬菜水果的拉曼光谱对比研究

本文通过改变不同的激光光源波长,测试分析了一系列蔬菜水果表面的拉曼谱。比较514.5nm和1064nm波长下的拉曼谱,发现514.5nm激发下许多蔬菜水果的拉曼谱均出现胡萝卜素的共振拉曼光谱,同时有很强的光荧光。更换成1064nm的近红外激光波长后,基本消除了光荧光和共振效应的影响,可用来测量蔬菜水果的有效成分,而514.5nm激发下只出现胡萝卜素的光谱,为区分蔬菜水果表面的外来物质,如农药,提供了很大的方便。     

Cr3+:Al2(WO4)3晶体的生长和光谱特性

采用顶部籽晶法从Na2WO4助熔剂体系生长出优质的Cr^3 ：Al2(WO4)3晶体,测定了吸收和荧光光谱,结果表明：Cr^3 离子在晶体中有两个宽且强的吸收带和一个微弱的吸收线,两宽带中心波长分别为422和595nm,还有两个较弱的吸收峰,其荧光峰值分别为684和663nm。其荧光宽带和一个较弱的荧光线峰并存,宽带范围为650～820nm,峰值波长为740nm,荧光线峰波长约为680nm,其强度较强。计算了晶场强度和Racah参数,其Dq／B=2．42,晶体属于中阶场介质。研究表明,Cr^3 ：Al2(WO4)3晶体具备可调谐激光晶体的基本光谱要求,且有良好的物化性能,可以实现宽频带可调谐激光输出。     

Evidence of Coordinate Field Index Influence on Upconversion Properties in Er3+ Doped Tellurite Glasses

Tellurite glasses doping the same concentration of Er³⁺ were prepared by conventional melting procedure, and their upconversion luminescences were measured. Two green emission bands at 521 nm and 550 nm and one red emission band at 657 nm were observed. This paper reported on the deduction of coordinate field index, which was proposed by deducing from Pauling's rules on the basis of Zachaiasen's random network theory, it was defined to the qualitative index that stand for the deviation of a given truly coordinate polyhedron from the hypothetical one. It can be used to rationalize the remarkable and regularity variation in the upconversion intensity in our prepared tellurite glasses.     

Optical studies of samarium-doped fluoride nanoparticles

Samarium-doped calcium fluoride (CaF₂) nanoparticles were synthesized by the co-precipitation method and characterized by powder X-ray diffraction (PXRD), Fourier transform infrared (FTIR) spectroscopy, scanning electron microscopy (SEM), optical absorption and photoluminescence (PL) techniques. The PXRD patterns confirmed the cubic crystallinity of the synthesized nanoparticles. The average particle size estimated using Scherer's formula was ～20?nm. The purity of the synthesized nanoparticles was confirmed by the FTIR spectrum. The morphological features studied using SEM revealed that the nanoparticles were agglomerated and porous. The optical absorption spectrum showed a strong and prominent absorption peak at ～264?nm and a weak one at ～212?nm. The PL spectrum showed broad and prominent emissions with peaks at ～387 and 532?nm along with weak emissions at 573 and 605?nm.